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27 Aug 2012: h. 1. 992. 24:3. 13-3. 58. D. ownl. oade. d fr. ... u. R. ev. F. luid. Mec. h. 1. 992. 24:3. 13-3.

3 Oct 2012: Department of Applied Mathematics. and Theoretical Physics. Goldstein Lab. Teaching. DAMTP Summer School on Fluid Dynamics of Sustainability and the Environment. Supplementary Reading (Biological Physics). The following is a collection of primary

19 Oct 2012: Instead, we adopt a new approach by adapting aclosure of Hinch and Leal [24] to d 2, yielding. ... G. Woodhouse and R. E. Goldstein (unpublished).[24] E. J. Hinch and L.

27 Dec 2012: 22]. Recent experimental evidence [24] is consistentwith the hypothesis of orbit flexibility and hydrodynamiccoupling as a possible origin of flagellar synchronization.At the same time, synchronization of an isolated pair is ... Custom-made rotation

19 Dec 2012: 24 • • 25. οργανώθηκε η κοινωνία μας τα τελευταία 40 χρόνια, αφετέ-ρου δε, της πληθώρας ευτελών μηνυμάτων που, με τη βοή-θεια Μέσων Μαζικής

2 Sep 2012: 15 OCTOBER 2010. 168101-2. surface [23], as well as a particular case of the ‘‘squirmer’’model [24]. ... Natl. Acad. Sci. U.S.A. 103, 8315. (2006).[24] J. R. Blake, J.

19 Jan 2012: We obtain ‘p 103 m, a value consistentwith the known range [13,14,24]. ... J. Hinch, J. Fluid Mech. 75,765 (1976). [24] H. Isambert et al., J.

3 Sep 2012: ThethroatdiameterD exhibitsanintriguingcrossover. R94 Invited Article. Figure 7. Collapse of the Möbius strip ‘throat’ [24]. ... c) Caustic visible from highly curvedsurface after the collapse of the Möbius strip surface [24].

2 Sep 2012: 2Program in Applied Mathematics, University of Arizona, Tucson, Arizona 85721, USA(Received 23 December 2003; published 24 August 2004). ... Rev.Lett. 71, 3975 (1993). [24] P. N. Segre, E. Herbolzheimer, and P.

2 Sep 2012: We obtain ‘p 103 m, a value consistentwith the known range [13,14,24]. ... J. Hinch, J. Fluid Mech. 75,765 (1976). [24] H. Isambert et al., J.

2 Sep 2012: Lipidmembranes do behave as two-dimensional f luids and can sup-port shear (24). ... Cole L, Orlovich DA, Ashford AE (1998) Fungal Genet Biol 24:86 –100.7.

2 Sep 2012: 4 A), representing either depletion or waste, alsoprovide spatially and temporally extended signals for the presenceof a colony, perhaps significant for intercolony communication, asin sexual induction (23) and quorum sensing (24), ... Michod, R. E. (2004

3 Sep 2012: See the article by Howard Berg, PHYSICSTODAY, January 2000, page 24.) The effect is not un-like a corkscrew pulling itself through the cork of awine bottle, except that the flagellum

10 Oct 2012: Therefore, (3.24) follows.The term Q1 is estimated using the bound. |Q1| = G. ... Fiα(λF) >= A Fiα (F) and the estimation (in. the spirit of (3.24)).

2 Sep 2012: O. Kessler, Annu. Rev. Fluid Mech. 24,313 (1992). [2] N. A.

22 Mar 2012: Evolving ideas of the stationary phase approximation [24], ourmethodsrequire explicit availability of more terms in the asymptotic expansion, leadingto the assumptions of non singularity of the matrix Aω and smoothness of ... 637–655. 24. E. M. Stein,

16 Jul 2012: λ1 1270.9 1103.4 1100.7 1099.8 1189.8λ2 26.39 48.24 46.37 44.92 28.13. ... 24] K. Frick, P. Marnitz, A. Munk, Statistical Multiresolution Estimation for Variational Imaging:With an Application in Poisson-Biophotonics, J.

2 Sep 2012: Rev. Fluid Mech. 24,313 (1992). [2] A. Einstein, Ann. Phys. (Leipzig) 17, 549 (1905).[3] P.

2 Sep 2012: 24,313 (1992). [2] W. F. Paxton et al., J. Am. Chem.

2 Sep 2012: solution to (24) subject to the boundary conditions is(Carslaw and Jaeger, 1959). ... computations. Fig. 2. The radial distribution function R0(r) for the parameter valuesP 1, N 8 , and Q 24.

12 Sep 2012: In a preliminary work [23, 24] we explored some mor-phological aspects of the fracture profiles obtained inplane-plane debonding experiments performed with gran-ular adhesives (crushed sand in an acrylic ... Van Damme, Fractals 1, 968 (1993).24. H. Van

2 Sep 2012: s L = 1.73, b = 1.31 rad / sL = 2.20, and c = 5.24 rad / s L = 3.11.

18 Oct 2012: R.; Jayaram, B.; Young,. M. A.; Beveridge, D. L.ReV. Comput. Chem.1997, 11, 317.(24) Kantor, Y.; Kardar, M.Phys.

2 Sep 2012: 1B), where η is the viscosity, and the distance betweenthe forces (24, 25). ... sions. Chem Phys 375:557–567.24. Batchelor GK (1970) The stress system in a suspension of force-free particles.

2 Sep 2012: Rev. Fluid Mech. 24,. 313 (1992).[3] X.-L. Wu and A. Libchaber, Phys.

2 Sep 2012: 24 and more complex numericalsimulations where these phenomena have been observed;see, e.g., Refs. ... Rev. Lett. 77, 1406 1996.37H. Daido, Physica D 91, 24 1996.38H.

2 Sep 2012: reinhardtii). Similar confine-ment can also occur in biofilms and in cellular transport near freesurfaces (24, 25), as well as in thin, mucous layers over ciliatedepithelia, such as line the human ... Phys Rev Lett 105:188101. 24. Oliver JK, Willis BL

2 Sep 2012: LabVIEW wasused to trigger the camera and control the LED light intensity time series.The temperature in the sample chamber was 24.5 0.5 C. ... Trends Cell Biol4:305–310. 24. Friedrich BM, Jülicher F (2007) Chemotaxis of sperm cells.

2 Sep 2012: A macroscopic scale model of bacterialflagellar bundlingMunJu Kim, James C. Bird, Annemarie J. Van Parys, Kenneth S. Breuer, and Thomas R. Powers. Division of Engineering, Brown University, Box D, Providence, RI 02912. Edited by Howard C. Berg,

3 Sep 2012: 24). So, by substituting (24) into (23), we have that. (P2M2)P1M1ϕ2 lBM2.

5 Sep 2012: 49) , and open 3D bulk suspensions (7, 18,24, 25), bacteria were confined in closed microfluidic chambers to. ... 6. Berg HC (1997) Motile behavior of bacteria. Phys Today 53:24–29.7.

2 Sep 2012: O. Kessler, Annu. Rev. Fluid Mech. 24,313 (1992). [7] T. Vicsek, A.

17 Apr 2012: 21:. 22:. 23:. 24:. 25:. 26:. 27:. 28:. 29:. 30:. 31:.

2 Sep 2012: equation and originally proposed to modelthe development of a breeding population [24]. ... 24. G.B. Arfken, H.J. Weber, Mathematical Methods for Physi-cists (Academic Press, San Diego, 1995).

20 Oct 2012: 3 Consistent reconstructions and oblique projections. We now consider the consistent sampling technique of [23, 24, 28, 55, 57]. ... An analysis of consistent reconstructions, which we shall recap and extend in 3.3, was given in[23, 24, 28].

2 Sep 2012: The latter point is more fully discussed by theRochester group (24, 40); one of the most important insightsemphasized by these researchers is that the capillary–muscle con-tact surface area is ... Cornish-Bowden,A. & Cardenas, M. L. (Plenum, New York),

3 Oct 2012: 60 74.605.082 1002.52 61.90 35.10 26.80 74.815.415 914.67 60.40 35.60 24.80 73.765.766 853.45 59.40

28 Feb 2012: 3.24) 2B2A4 2[(. κ2 2) 2. ]BA3 2 2. (κ2 2. ... Nevertheless, from (3.24) the Re 0 limit is observedto be consistent with (3.12) obtained for Re = 0 and M = 1.

3 Oct 2012: Rev. Lett. 24, 156–159(1970). 8. G. M. Gibson, J. Leach, S. ... We use the power spectral density method [24] within arecently suggested optimized calibration protocol [26, 27].

2 Sep 2012: See the article by Howard Berg, PHYSICSTODAY, January 2000, page 24.) The effect is not un-like a corkscrew pulling itself through the cork of awine bottle, except that the flagellum

3 Sep 2012: tracking code,24 or manually selected on each image using. ImageJ software,25 depending on the contrast. ... 23 E. Sackmann and R. F. Bruinsma, ChemPhysChem, 2002, 3,262–269. 24 J.

2 Sep 2012: Julicher, New J. Phys., 2000, 2, 24.18 J. R. Blake and M. ... Rev. Lett., 2009, 102, 168101.24 M. Polin, I. Tuval, K. Drescher, J.

2 Sep 2012: 24 OCTOBER 2008. 178102-3. [Fig. 4(b)] is dominated by a 1= dependence, leading to avery strong 3 scaling as the amplitude of the streamfunction approaches zero. ... G. Bessoth, A. J. deMello, and A. Manz, Anal. Commun. 36, 213 (1999).[24] J.

28 Feb 2012: On rapid computation of expansions in ultraspherical. polynomials. Maŕıa José CanteroDepartamento de Matemática Aplicada. Centro Politécnico Superior de IngenierosUniversidad de Zaragoza. Spain. Arieh IserlesDepartment of Applied

25 Apr 2012: from [1],. ẍµ1(1 x2)ẋ vx = α1ẏ α2y ι(t). 24. Figure 4.1: Equation (4.1).

28 Feb 2012: 24. another generating function,. Ψ(t) =. n=0. φn(z)tn. =. [1. (2c 1)α z(αz)2 4α|c|2z.

28 Feb 2012: 24. n Z+. Given the quindiagonal structure of C, we have.

27 May 2012: carteri isachieved by cells at the bend points, which undergo adistinct transition in cell shape [20,22-24,26-29]. ... More-over, concerted movements of cells with respect to theCB system are crucial for the process of inversion in V.carteri

2 Aug 2012: Then, if wetake. g = (q>q)γ/2 (24). for an appropriate choice of γ, we have.

2 Sep 2012: not new. In a prescient article, Finlayson & Scriven (24) argued that biological matter.